The present invention relates to endoscopes for examining the interior of a body, and particularly to endoscopes of the optical-fiber type.
The invention is particularly useful for the real-time, in vivo measurements of the ciliary beat frequency (CBF) of the human fallopian tube during laparotomy or laparoscopy. The invention is therefore described below with respect to such application, but it will be appreciated, as will also be indicated below, that the invention could advantageously be used in other applications as well, particularly in the ENT (ear, nose, throat) field.
Cilia are tiny hairlike appendages, about 0.25 μm in diameter, that are built from bundles of parallel microtubules. They extend from many kinds of epithelial cells and are found in most animal species and in some lower plants. Their primary function is to move fluid over the surface of cells, or to propel cells through fluid. Impairment of ciliary activity in animals may produce infertility by interference with ovum pickup by the fimbria and transport through the fallopian tubes. For this reason, evaulation of the ciliary beating can serve as a viable tool for medical evaluation and treatment of infertile women.
Also, the mucociliary system is one of the most important airway defense mechanisms, and knowledge of the ciliary beat frequency is important in understanding this system. Drugs, allergies, and upper respiratory infections are known to affect the ciliary mobility.
A number of techniques have been described in the literature for measurement and evaluation of CBF. One known technique is based on the detection of back-scatted light (from ciliary epithels) and is described in Lee WI, Verdugo P. Laser Scattering Spectroscopy: A New Application in the Study of Ciliary Activity. Biophys J 1976; 16:1115-9. However, one of the problems in real-time measurement of ciliary motion, particularly when using a back-scattered light technique, is the spurious low frequency signals originating from breathing and heartbeat movements of the patient and hand movements of the surgeon. These artifacts substantially reduce the signal-to-noise ratio.
An object of the present invention is to provide an improved endoscope for examining the interior of a body based on the detection of light back-scattered from the interior of the body being examined. Another object of the present invention is to provide an improved endoscope particularly useful in measuring and evaluating CBF in a real-time manner, but which may be used in other applications.
According to the present invention, there is provided an endoscope for examining the interior of a body, comprising: a long slender tube having a probe tip at one end insertable into the body to be examined; first, second and third optical fibers extending through the tube to the probe tip; a source of light at the opposite end of the tube aligned with the first optical fiber for transmitting light into the body via the probe tip; light detectors at the opposite end of the tube, one in alignment with each of the second and third optical fibers, for receiving light transmitted therethrough back-scattered from the interior of the body; and differential measuring means for differentially measuring the outputs of the two detectors such as to substantially cancel out artifacts and to increase the signal-to-noise ratio.
According to further features in the preferred embodiment of the invention described below, the first optical fiber has a small optical core such that it operates as a single mode fiber; the second and third optical fibers have larger optical cores than the first optical fiber and operate as multi-mode fibers.
An endoscope constructed in accordance with the foregoing features has been found to substantially reduce the motion artifacts due to breathing and heartbeat movements of the patient and hand movements of the surgeon. By using two collecting optical fibers, the motion artifacts tend to affect both optical fibers in the same manner, and thus may be cancelled out by the differential treatment of the measurements; on the other hand, fluctuations resulting from ciliary motion detected in two different coherence areas produce uncorrelated fluctuating signals and thereby tend to increase the signal. In addition, the use of a single-mode fiber of very small core diameter produces a light intensity profile close to a smooth Gaussian profile, independent of fiber flexing, and thereby tends to avoid speckle pattern fluctuations due to fiber movements. The low coherence of the back-scattered light is not significantly affected by the flexing of the multimode fibers.
Further features and advantages of the invention will be apparent from the description below.
The invention is herein described, by way of example only, with reference to the accompanying drawings, wherein:
FIG. 1 is a block diagram illustrating one form of endoscope apparatus constructed in accordance with the present invention for examining the interior of a body;
FIG. 2 is a block diagram illustrating the electrical circuit in the apparatus of FIG. 1;
FIG. 3 more particularly illustrates the endoscopic probe in the apparatus of FIG. 1;
FIG. 4 more particularly illustrates the probe tip in the endoscope of FIG. 3;
FIG. 5 is an enlarged sectional view more particularly illustrating the end face of the probe tip in the endoscope of FIGS. 3 and 4;
FIG. 6 illustrates an endoscope particularly useful for measuring CBF in the middle ear;
FIG. 7 is an enlarged fragmentary view more particularly illustrating the probe tip in the endoscope of FIG. 6;
FIG. 8 illustrates an endoscope particularly useful for measuring CBF in the breathing tracts; and
FIG. 9 illustrates a sample of a display produced as a result of CBF measurements using the apparatus of FIG. 1.
The apparatus illustrated in the drawings is particularly useful for measuring CBF (ciliary beat frequency) in laparoscopy or laparotomy (FIGS. 2 and 3), or in the middle ear (FIGS. 6 and 7) or in the breathing tracts (FIG. 8).
As shown in FIG. 1, the apparatus includes an endoscope in the form of a long, slender,rigid tube 2 insertable at one end into the body to be examined. The opposite end of therigid tube 2 is connected via a flexible sleeve 4 to a source oflight 6 for illuminating the interior of the body to be examined, and alight measuring circuit 8 for measuring the back-scattered light from the interior of the examined body.
The source oflight 6 is a laser. It is coupled via afiber coupler 10 to the end of asingle mode fiber 11 extending via the flexible sleeve 4 into theendoscope 2 for transmitting the light from the laser to the examined body.Endoscope 2 and the flexible sleeve 4 include two furtheroptical fibers 12, 13; these are multimode fibers and are connected to thelight measuring circuit 8 for transmitting thereto the back-scattered light from the examined region.
Thelight measuring circuit 8 is more particularly illustrated in FIG. 2. It includes: twolight detectors 14, 16, one for each of the two light-collecting fibers 12, 13; twopreamplifiers 18, 20 for preamplifying the outputs of the twolight detectors 14, 16; and adifferential amplifier 22 for receiving the amplified outputs of the two light detectors. The output ofdifferential amplifier 22 thus corresponds to the momentary difference in the amount of light received by the twolight detectors 14, 16 from theirrespective collector fibers 12, 13.
The output fromdifferential amplifier 22 is fed to a bandpass filter andgain control unit 24 to amplify the range of frequencies of typical cilia beats (0.5-30 Hz). The gain ofunit 24 is controlled by a variable-gain potentiometer 26 (FIG. 1). As further shown in FIG. 1, the output from thelight measuring circuit 8 is fed, via an analog-to-digital converter 28 to adigital processor 30 for processing and display via adisplay unit 32.
Laser 6 is preferably alow power 2 mW He--Ne laser, or a dye laser. It is coupled by a single-mode fiber coupler 10 to the single-mode illuminating fiber 11 leading from the flexible sleeve 4 into theendoscope 2. FIGS. 3-5 more particularly illustrate the structure of the endoscope.
Thus, as shown particularly in FIG. 5, theendoscope 2 includes a long outerrigid tube 30, preferably of stainless steel, enclosing the threeoptical fibers 11, 12 and 13. At the probe tip 2a, the fibers are embedded in anepoxy resin 32 whose outer face is polished. The probe tip is thus sealed to prevent air leakage and is sterilizable.
Theilluminating fiber 11 is a single-mode fiber, including an inner core 11a (FIG. 5) of very small diameter, anouter cladding 11b, and an outer jacket (not shown in FIG. 5). On the other hand, the two collectingfibers 12, 13, include large-diameter cores 12a, 13a,claddings 12b, 13b, and outer jackets (not shown in FIG. 5). All three fibers, extend to the end of therigid tube 2 constituting the probe tip insertable into the examined region, which probe tip has a flat, optically polished end face (FIG. 5). As shown in FIG. 4, the threeoptical fibers 11, 12, 13 are stripped of their jackets at their ends so that only their cores and claddings are exposed, and are close to each other, at the end face (FIG. 5) of the probe tip 2a.
The diameter of the core 11a of theilluminating fiber 11 is so small that it can sustain only the lowest transversal laser mode. Under these conditions, the laser intensity profile is close to a smooth Gaussian and is independent of fiber flexing. On the other hand, the cores of the two back-scatteredlight collecting fibers 12, 13 are of substantially larger diameter and have a relatively high numerical aperture (e.g., 0.316) so as to serve as multimode fibers. They collect a large fraction of the scattered light and transmit such light to theirrespective light detectors 14, 16.
Eachlight detector 14, 16 is preferably a photodiode and includes anarrow bandwidth filter 14a, 16a (FIG. 2) for passing only the wavelength of thelaser 6, thereby eliminating the effects of surgical ambient or other extraneous white light not supplied from the laser.
As indicated earlier, utilizing two collecting optical fibers reduces the artifacts originating from breathing and heartbeat motions of the patient and hand motions of the surgeon or physician since such motions would affect both optical fibers in the same manner and thus tend to cancel out by thedifferential amplifier 22. On the other hand, fluctuations resulting from ciliary motion are detected by the two collector fibers in two different laser coherence areas, which are random and therefore do not cancel out. As a result, a relatively high signal-to-noise ratio is produced at the output of thedifferential amplifier 22.
As one example, therigid steel tube 30 of theendoscope 2 may have an outer diameter of 5 mm and an inner diameter of 4 mm; theilluminating fiber 11 may have a core diameter of 4 microns, and a cladding diameter of 125 microns, and a jacket diameter of 250 microns; and each of the twocollector fibers 12, 13 may have a core diameter of 100 microns, a cladding diameter of 200 microns, and a jacket diameter of 1,000 microns. The length of the rigidstainless steel tube 30 of theendoscope 2 may be 35 cm, and the length of the flexible sleeve 4 connecting theendoscope 2 to thelaser 6 andlight measuring circuit 8 may be about 1.5 M.
FIGS. 6 and 7 illustrate a modification in the construction of the endoscope, therein designated 102, particularly useful for CBF measurements in the middle ear. This construction also includes the threeoptical fibers 111, 112, 113, enclosed within arigid tube 102. Here, however, the end of thetube 102 constituting theprobe tip 102a is reduced in diameter, e.g., to about 1 mm, so as to facilitate its insertion through the hole in a button inserted in the ear membrane, to release fluid accumulating during ear infections common in growing children.
FIG. 8 illustrates an endoscope particularly useful for measuring CBF in the breathing tracts. This arrangement also includes the threeoptical fibers 211, 212, 213, as described above, except that they are enclosed in aflexible tube 202 for insertion into the breathing tract, or through the channel of aflexible endoscope 202a.
Filters 14a, 16a in front of thelight detectors 14, 16 (FIG. 2) may have maximum transmission at 633 nm, thereby matching the wavelength of the He--Ne laser 6 to eliminate the effects of ambient light.Differential amplifier 22 may have a high-pass sharp frequency cutoff at 0.5 Hz to prevent saturation of the amplifiers because of slow movements.
Processor 30 may be a personal computer which samples the output signals from the analog-to-digital converter 28 according to user-specified sampling parameters, and stores the data in the computer memory in a direct memory access mode. This enables accumulating and processing the data simultaneously. User-chosen parameters would include: averaging time (in minutes), the number of sampling points N (e.g., 32, 64, 128, 256, or 512), and maximum frequency (cycles/sec.). The maximum frequency (Fmax) determines the sampling rate, which is set at 2×Fmax. For each array of N sampled data points, Fourier transformation and squaring yield the power spectrum of all the frequencies up to Fmax. A larger number of sampling points N gives the same overall shape of the power spectrum at higher frequency resolution, but obviously takes longer to sample and calculate, and therefore yields a slower real-time response to the operator. The averaging time determines how many separate power spectra will be averaged in the final power spectrum.
To establish the sensitivity of CBF measurements, and the effects of probe movements and proximity to the surface, experiments were first performed in vitro on human upper respiratory tract cilia obtained by nasal smear, or slices of chicken trachea immersed in medium. Photometric microscopy served as a reference method to which observations of the laser instrument were compared under well controlled conditions.
In the second stage of the study, measurements were performed on excised human oviducts which were removed during total abdominal hysterectomy, and put into tissue culture medium (Ham's F-10). CBF measurements were performed within few minutes after the tubes were removed, since a decline in CBF was observed as a function of time. It was also observed that the CBF had declined rapidly when the medium temperature decreased. The optimal results were obtained when the probe touched gently the fimbria and when the probe was inserted into the ampulla without pressing the oviductal walls.
The parameters that gave an optimum signal to noise ratio with fast response time were found to be: average time of 0.6 min, 128 sampling points, and maximum frequency of 20 Hz, giving a display of updated spectrum ever 3.2 seconds, and final frequency power spectrum averaged for 11 spectra. Nine measurements of CBF of fimbria of excised human fallopian tubes were made with these parameters. The mean ± SEM value for the CBF was 5.9±0.5 (4.7-8.4) Hz.
In the next stage of the study, CBF of intact human oviducts was measured. Measurements were done only in menstruating women undergoing laparotomy or laparoscopy. CBF measurements were performed during laparatomy in 65 cases, during laparoscopy in 13 cases, during cesarean section in 9 cases. In 49 cases of the laparotomy group, total abdominal hysterectomy was done because of uterine myoma. In 16 cases, the indication for laparotomy was ovarian tumor and ovarian cystectomy was performed. The indication for 7 laparoscopies was tubal sterilization, and for 6 laparoscopies was infertility investigation.
The mean ± SD (standard deviation) of 142 measurements of CBF in the fimbria was 5.45±1.3 Hz and in 73 measurements in the ampulla 4.95±1.7 Hz, P (probability) <0.05.
FIG. 9 illustrates the results as displayed in the computer monitor (32, FIG. 1) which was obtained during laparoscopy of one of the women examined (Case No.2), utilizing the parameters specified in FIG. 9. The obvious frequency peak around 4.7 Hz pointed by the cursor corresponds to the CBF.
The described method was also used to study the mucociliary activity in vivo of 17 patients with a deviated nasal septum, 7 patients with allergic rhinitis, and 17 healthy persons. In this study patients suffering from purulent discharge from the nose were not investigated. The healthy persons were patients examined in the outpatient clinic, without any nasal complaints.
The patient sat relaxed on an upright chair facing the examiner. No local anesthesia was given in order not to affect the ciliary activity. The probe was introduced in each nostril under visual inspection, sounding the anterior border of the inferior caudal. The optimal signals were obtained when the probe touched gently the nasal mucosa without pressing the nasal walls which may impair mechanically cilia beating. The time of each measurement ranged for 0.4-0.6 minutes.
The mean ± SE of CBF measurements in normal cases was 7.7±0.5 Hz. The mean CBF in cases with allergic rhinitis was 5.1±0.2 Hz (t=2.7 P<0.05) and in case of septum deviation 5.4±0.3 Hz (t=2.7 P<0.05).
While the invention has been described with respect to measuring CBF in laparoscopy or laparotomy, in the bronchi or trachea, or in the middle ear, it will be appreciated that the invention could be used in many other applications.